JPS6156956B2 - - Google Patents
Info
- Publication number
- JPS6156956B2 JPS6156956B2 JP12144380A JP12144380A JPS6156956B2 JP S6156956 B2 JPS6156956 B2 JP S6156956B2 JP 12144380 A JP12144380 A JP 12144380A JP 12144380 A JP12144380 A JP 12144380A JP S6156956 B2 JPS6156956 B2 JP S6156956B2
- Authority
- JP
- Japan
- Prior art keywords
- humidity
- resistance
- resistor
- bridge
- resistance value
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000001514 detection method Methods 0.000 claims description 14
- 238000005259 measurement Methods 0.000 claims description 7
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 claims description 3
- 239000000463 material Substances 0.000 claims description 2
- 229910052751 metal Inorganic materials 0.000 claims description 2
- 239000002184 metal Substances 0.000 claims description 2
- 238000005245 sintering Methods 0.000 claims description 2
- 230000008878 coupling Effects 0.000 claims 1
- 238000010168 coupling process Methods 0.000 claims 1
- 238000005859 coupling reaction Methods 0.000 claims 1
- 230000007423 decrease Effects 0.000 description 8
- 238000010586 diagram Methods 0.000 description 3
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 239000011810 insulating material Substances 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 1
- 238000010981 drying operation Methods 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P5/00—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft
- G01P5/10—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring thermal variables
- G01P5/12—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring thermal variables using variation of resistance of a heated conductor
Landscapes
- Engineering & Computer Science (AREA)
- Aviation & Aerospace Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Testing Or Calibration Of Command Recording Devices (AREA)
- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
Description
【発明の詳細な説明】
本発明は気体の流速例えば風速と、その気体の
湿度とを同時に測定することが出来る新規な流速
及び湿度同時測定装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a novel flow velocity and humidity simultaneous measurement device that can simultaneously measure the flow velocity of a gas, such as wind velocity, and the humidity of the gas.
気体等の流速並びに湿度の測定を個々に行う装
置は既に多数提案されている。 Many devices have already been proposed that individually measure the flow velocity and humidity of gas and the like.
然しながら流速と湿度との両者を同時に、然か
も一個の検出素子をもつて測定する方法は提案さ
れていなかつた。 However, no method has been proposed in which both flow velocity and humidity can be measured at the same time using a single detection element.
本発明は新規な技術的思想に基づいて提案され
たものであつて、気体の流速と、その湿度とを同
時に測定し得る極めて有効な流速及び湿度同時測
定装置であつて、以下実施例に従つて説明する。 The present invention has been proposed based on a novel technical idea, and is an extremely effective flow velocity and humidity simultaneous measuring device that can simultaneously measure the flow velocity of gas and its humidity. I will explain.
第1図は検出素子Sの一部切欠き概略図であつ
て、1は抵抗線を示し、例えば白金等の抵抗温度
係数の比較的大きな金属の細線を用い、その線径
は例えば20〜50μmφ程度のものである。2は前
記抵抗線1を被覆する耐熱絶縁材である。4は前
記抵抗線及びその被覆材を芯としてその上に焼結
形成された金属酸化物の多孔質感湿抵抗体であつ
て、例えばその両端には端子3a及び3bが埋設
される。1a及び1bは前記抵抗線1の端子を示
す。 FIG. 1 is a partially cutaway schematic diagram of the detection element S, in which 1 indicates a resistance wire, for example, a fine wire made of a metal with a relatively large temperature coefficient of resistance, such as platinum, and the wire diameter is, for example, 20 to 50 μmφ. It is of a certain degree. 2 is a heat-resistant insulating material that covers the resistance wire 1. Reference numeral 4 denotes a porous metal oxide moisture resistor formed by sintering the resistance wire and its covering material as a core, and terminals 3a and 3b are embedded at both ends thereof, for example. 1a and 1b indicate terminals of the resistance wire 1.
尚、感湿抵抗体4は抵抗線1と熱結合され、常
に後述する所定の温度を保つものとする。 It is assumed that the humidity sensitive resistor 4 is thermally coupled to the resistance wire 1 and always maintains a predetermined temperature, which will be described later.
斯かる構成になる検出素子Sは感湿抵抗体4が
吸湿することによつて、その端子3a,3b間の
抵抗値が低下するものである。 In the detection element S having such a configuration, the resistance value between the terminals 3a and 3b decreases when the moisture-sensitive resistor 4 absorbs moisture.
その湿度―抵抗特性の代表例を第2図に示す。
第3図は実施例の具体的回路を例示したもので、
前記詳述した検出素子Sは点線で画したる部分で
あつて、前記抵抗線1は抵抗R1にて、又感湿抵
抗体4は抵抗4′なる記号にてそれぞれ置き替え
られ図示されている。 A typical example of its humidity-resistance characteristics is shown in Figure 2.
FIG. 3 illustrates a specific circuit of the embodiment.
The above-mentioned detailed detection element S is a part delineated by a dotted line, and the resistance line 1 is shown replaced by a resistance R1, and the moisture-sensitive resistor 4 is replaced by a resistance 4'. .
而して前記抵抗R1及び固定抵抗R2,R3,
R4によつてブリツジ回路が構成され、a点及び
b点の電位変化は増巾回路5に入力され、その出
力からはブリツジ回路が平衡を保つよう、該ブリ
ツジ回路に電流Iが帰還される。 The resistor R1 and the fixed resistors R2, R3,
A bridge circuit is constituted by R4, and potential changes at points a and b are input to an amplifying circuit 5, and from its output, a current I is fed back to the bridge circuit so that the bridge circuit maintains balance.
一方湿度によつて変化する抵抗4′は、その両
端子が抵抗値検出回路6に接続され、その値を湿
度表示器7によつて湿度表示するよう構成されて
いる。 On the other hand, both terminals of the resistor 4', which changes depending on the humidity, are connected to a resistance value detection circuit 6, and the humidity display 7 displays the value of the resistor 4'.
尚、8は後述するように流速値を表示する流速
表示器である。 Note that 8 is a flow rate indicator that displays a flow rate value as described later.
而して前記ブリツジを構成する各辺の抵抗の値
は、R2=224Ω、R3=200Ω、R4=20Ω程度
であつて、R1の値は後述する(2)式より22.4Ωと
なる。尚、抵抗R1の抵抗温度係数αは0.004程
度である。 The resistance values on each side of the bridge are approximately R2 = 224Ω, R3 = 200Ω, and R4 = 20Ω, and the value of R1 is 22.4Ω from equation (2) described later. Note that the resistance temperature coefficient α of the resistor R1 is approximately 0.004.
斯くの如き構成に於いて、0℃に於ける抵抗R
1の抵抗値をR0、その抵抗温度係数をα、その
温度をTとすれば
R1=R0(1+αT) (1)
が成り立つ。 In such a configuration, the resistance R at 0°C
If the resistance value of 1 is R0, its temperature coefficient of resistance is α, and its temperature is T, then R1=R0(1+αT) (1) holds true.
又、抵抗R1,R2,R3,R4で構成される
ブリツジの平衡条件は
R1・R3=R2・R4 (2)
であり、
いま抵抗R1が加熱されておらず、その抵抗値が
低く
R1・R3<R2・R4 (3)
なる場合、第3図のa点の電位がb点より低く
なる。 Also, the equilibrium condition of the bridge composed of resistors R1, R2, R3, and R4 is R1・R3=R2・R4 (2), and now resistor R1 is not heated and its resistance value is low. <R2·R4 (3) If so, the potential at point a in FIG. 3 becomes lower than point b.
a点には増巾器5の反転入力端子が、又b点に
は非反転入力端子がそれぞれ接続されているか
ら、a点の電位が低くなると増巾器5の出力電流
Iが増加し、抵抗R1が加熱されることになる。
逆に抵抗R1が加熱され過ぎると
R1・R3>R2・R4 (4)
となり、斯かる場合a点の電位はb点より高く
なり、電流Iが減少する。 Since the inverting input terminal of the amplifier 5 is connected to point a, and the non-inverting input terminal is connected to point b, when the potential at point a decreases, the output current I of the amplifier 5 increases, Resistor R1 will be heated.
Conversely, if the resistor R1 is heated too much, R1.R3>R2.R4 (4), and in this case, the potential at point a becomes higher than point b, and the current I decreases.
斯かる作動によつてブリツジの平衡条件、(2)式
が自動的に満足され、R1の抵抗値が一定とな
る。その結果、(1)式によつて示される如く、抵抗
R1の温度が一定に保たれるものである。尚、R
0=20Ωとする。 Through this operation, the bridge equilibrium condition, equation (2), is automatically satisfied, and the resistance value of R1 becomes constant. As a result, as shown by equation (1), the temperature of the resistor R1 is kept constant. Furthermore, R
0=20Ω.
而してブリツジの各辺の抵抗値が前記した値で
あるとすると、この時の抵抗R1の温度は、(1)式
より30℃となる。 Assuming that the resistance values on each side of the bridge are the values described above, the temperature of the resistor R1 at this time will be 30° C. from equation (1).
すなわち、実施例では抵抗R1と感湿抵抗体
4′とは熱結合されているから、該抵抗体4′の温
度は常に30℃に保たれるものである。 That is, in the embodiment, since the resistor R1 and the humidity sensitive resistor 4' are thermally coupled, the temperature of the resistor 4' is always maintained at 30°C.
次に湿度に関して説明すると、水の飽和気圧は
零囲気温度20℃に於いて17.53mmHgであり、これ
が30℃になると31.83mmHgとなる。相対湿度は気
体中の水蒸気圧と、その気体と同じ温度の飽和水
蒸気圧との比を百分率で表わした量である。 Next, regarding humidity, the saturated pressure of water is 17.53 mmHg at a zero ambient temperature of 20°C, and becomes 31.83mmHg at 30°C. Relative humidity is the ratio of the water vapor pressure in a gas to the saturated water vapor pressure at the same temperature as the gas, expressed as a percentage.
従つて実施例の場合、雰囲気温度20℃で相対湿
度が100%であるとしても、感湿抵抗体4′の温度
が前記の如く30℃に保たれているため、該抵抗体
4′自体は等価的に
17.53/31.83×100=55.07 …(5)
すなわち、約55%の湿度雰囲気中にあることに
相当する。 Therefore, in the case of the embodiment, even if the ambient temperature is 20°C and the relative humidity is 100%, the temperature of the humidity-sensitive resistor 4' is maintained at 30°C as described above, so the resistor 4' itself Equivalently, 17.53/31.83×100=55.07 (5) That is, it corresponds to being in an atmosphere with a humidity of approximately 55%.
斯かることは第2図特性図からもわかるよう
に、湿度―抵抗特性の直線性の良好な範囲で湿度
の検出を行わせることが出来、これによつて高い
測定精度が得られることになる。 As can be seen from the characteristic diagram in Figure 2, this allows humidity to be detected within a range where the linearity of the humidity-resistance characteristics is good, thereby providing high measurement accuracy. .
次に流速の測定作動に付いて説明すると、前記
した如く実施例回路が作動すると(2)式が満足さ
れ、従つて抵抗R1の値は一定となる。尚、抵抗
R1は雰囲気温度よりも常に高い温度にて一定と
なるよう回路の定数が選定されている。 Next, the operation of measuring the flow velocity will be explained. When the circuit of the embodiment operates as described above, equation (2) is satisfied, and therefore the value of the resistor R1 becomes constant. Note that the circuit constants of the resistor R1 are selected so that the resistor R1 remains constant at a temperature that is always higher than the ambient temperature.
抵抗R1への電流、すなわちブリツジに供給さ
れる電流Iは、抵抗R1が一定の温度となるよう
制御されており、前記電流によつて発生した熱は
周囲の気体中に放散される。抵抗R1の周囲の気
体(正確には感湿抵抗体を介した気体)が流動し
ている場合、すなわち気体が或る速度で移動して
いる場合には放散熱量が増加し、従つて前記電流
Iも増大する。 The current to the resistor R1, ie the current I supplied to the bridge, is controlled so that the resistor R1 is at a constant temperature, and the heat generated by said current is dissipated into the surrounding gas. When the gas around the resistor R1 (more precisely, the gas passing through the moisture-sensitive resistor) is flowing, that is, when the gas is moving at a certain speed, the amount of heat dissipated increases, and therefore the current I also increases.
流速が高くなつた場合には前記抵抗R1から放
散される熱量が増加し、従つて抵抗R1は冷却さ
れる。冷却されるとその抵抗値が低下し(3)式とな
る。 When the flow rate increases, the amount of heat dissipated from the resistor R1 increases and thus the resistor R1 is cooled. When cooled, its resistance value decreases, resulting in equation (3).
斯かる状態になると回路の作動によつて電流I
が増大し、抵抗R1が加熱される。すると再び(2)
式の条件が満足される。 In such a state, the current I increases due to the operation of the circuit.
increases, and the resistor R1 is heated. Then again (2)
The condition of Eq.
流速が低くなつた場合には抵抗R1から放散さ
れる熱量が減少し、従つて該抵抗の温度は上昇す
る。上昇するとその抵抗値は高く、従つて(4)式と
なり電流Iが減少して抵抗R1の温度が低下し、
再び(2)式が満足されることになる。 When the flow rate decreases, the amount of heat dissipated from resistor R1 decreases, and therefore the temperature of the resistor increases. As it rises, its resistance value becomes high, so the current I decreases and the temperature of the resistor R1 decreases, as shown in equation (4).
Equation (2) is satisfied again.
斯くの如く流速が変化すると、それに従つて電
流Iが変化する。実施例ではこの電流変化に相当
する信号を取り出して流速表示器8を駆動させ、
その指示値から流速値を知ることが出来るもので
ある。尚、以上の説明では湿度の測定作動と、流
速の測定作動とをそれぞれ分けて説明したが、実
際にはこれらは同時に行われ、湿度表示器7及び
流速表示器8とによつて被測定気体の湿度と流速
とを同時に測定することが出来るものである。 When the flow velocity changes in this way, the current I changes accordingly. In the embodiment, a signal corresponding to this current change is extracted to drive the flow rate indicator 8,
The flow velocity value can be determined from the indicated value. In the above explanation, the humidity measurement operation and the flow rate measurement operation were explained separately, but in reality, these are performed at the same time, and the humidity indicator 7 and the flow rate indicator 8 are used to measure the gas to be measured. It is possible to measure the humidity and flow velocity of the air at the same time.
本発明は以上に詳述した如く、比較的簡単な構
成にも拘らず、湿度と流速との二つの測定が同時
に行え、使用上極めて大なる効果を有している。
更に実施例に於いては感湿抵抗体が常に一定温度
に加熱されているから、長時間の高湿度測定時に
於いて感湿抵抗体の乾燥操作が従来方法のものと
比べて少なくてすみ、この点に於いても本発明は
優れた効果を有している。 As described in detail above, the present invention, despite its relatively simple structure, can simultaneously perform two measurements of humidity and flow rate, and has extremely great effects in use.
Furthermore, in the embodiment, since the humidity-sensitive resistor is always heated to a constant temperature, the drying operation of the humidity-sensitive resistor during long-term high-humidity measurements is less than that required in the conventional method. The present invention has excellent effects in this respect as well.
第1図は本発明の一実施例による流速及び湿度
同時測定装置に用いる検出素子の一例を示す一部
切欠断面図、第2図はこの検出素子の湿度に対す
る抵抗値の変化を示すグラフ、第3図は本発明の
一実施例による流速及び湿度同時測定装置の構成
を示す回路図である。
S…検出素子、1…抵抗線、1a,1b…端
子、2…耐熱絶縁材、3a,3b…端子、4…感
湿抵抗体、R1,R2,R3,R4,r…抵抗、
4′…感湿抵抗体、5…増幅器、6…抵抗値検出
回路、7…湿度表示器、8…流速表示器。
FIG. 1 is a partially cutaway cross-sectional view showing an example of a detection element used in a simultaneous flow velocity and humidity measuring device according to an embodiment of the present invention, and FIG. 2 is a graph showing changes in resistance value of this detection element with respect to humidity. FIG. 3 is a circuit diagram showing the configuration of a simultaneous flow rate and humidity measuring device according to an embodiment of the present invention. S...Detection element, 1...Resistance wire, 1a, 1b...Terminal, 2...Heat-resistant insulating material, 3a, 3b...Terminal, 4...Moisture-sensitive resistor, R1, R2, R3, R4, r...Resistance,
4'...Humidity sensitive resistor, 5...Amplifier, 6...Resistance value detection circuit, 7...Humidity indicator, 8...Flow rate indicator.
Claims (1)
線を感湿体で包み込んで熱結合し、該感湿体の両
端に端子を設けて構成された検出素子と、 前記検出素子内の抵抗線を一辺に有するブリツ
ジ回路と、 前記ブリツジ回路の一対の端子が入力端に接続
され前記ブリツジ回路に帰還電流を供給すること
によりブリツジを平衡に保つ帰還増幅器と、 前記帰還増幅器の帰還出力に対応した流速を表
示する流速表示器と、 前記ブリツジの平衡により所定温度に保たれた
前記感湿体の抵抗値を検出する抵抗値検出回路
と、 前記抵抗値検出回路の抵抗値出力によつて前記
感湿抵抗体の周囲の湿度を表示する湿度表示器
と、を具備することを特徴とする流速及び湿度同
時測定装置。 2 前記検出素子は、被覆された抵抗線を芯とし
てその周囲に多孔質感湿体を焼結して形成したも
のであることを特徴とする特許請求の範囲第1項
記載の流速及び湿度同時測定装置。 3 前記感湿抵抗体の抵抗線は、温度抵抗係数の
大きい金属線であることを特徴とする特許請求の
範囲第1項記載の流速及び湿度同時測定装置。 4 前記抵抗線は、白金線であることを特徴とす
る特許請求の範囲第3項記載の流速及び湿度同時
測定装置。[Scope of Claims] 1. A detection element configured by wrapping and thermally coupling a coated resistance wire having a resistance value depending on temperature with a moisture sensitive body, and providing terminals at both ends of the moisture sensitive body; a bridge circuit having a resistance wire in a detection element on one side; a feedback amplifier having a pair of terminals of the bridge circuit connected to an input terminal and keeping the bridge in balance by supplying a feedback current to the bridge circuit; and the feedback amplifier. a flow velocity indicator that displays the flow velocity corresponding to the feedback output of the bridge; a resistance value detection circuit that detects the resistance value of the moisture sensitive body maintained at a predetermined temperature by the equilibrium of the bridge; and a resistance value of the resistance value detection circuit. A flow rate and humidity simultaneous measuring device comprising: a humidity indicator that displays the humidity around the humidity sensitive resistor by output. 2. Simultaneous measurement of flow velocity and humidity according to claim 1, wherein the detection element is formed by sintering a porous moisture material around a coated resistance wire as a core. Device. 3. The flow velocity and humidity simultaneous measuring device according to claim 1, wherein the resistance wire of the humidity-sensitive resistor is a metal wire having a large temperature resistance coefficient. 4. The flow rate and humidity simultaneous measuring device according to claim 3, wherein the resistance wire is a platinum wire.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12144380A JPS5745464A (en) | 1980-09-01 | 1980-09-01 | Measuring method for flow speed and humidity |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12144380A JPS5745464A (en) | 1980-09-01 | 1980-09-01 | Measuring method for flow speed and humidity |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5745464A JPS5745464A (en) | 1982-03-15 |
| JPS6156956B2 true JPS6156956B2 (en) | 1986-12-04 |
Family
ID=14811260
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12144380A Granted JPS5745464A (en) | 1980-09-01 | 1980-09-01 | Measuring method for flow speed and humidity |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5745464A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE102013103388B3 (en) * | 2013-04-05 | 2014-09-25 | Chemec Gmbh | Device for measuring the thermal conductivity of gas components of a gas mixture |
-
1980
- 1980-09-01 JP JP12144380A patent/JPS5745464A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5745464A (en) | 1982-03-15 |
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